Achieve a new level of precision in your spectral analysis with the JINSP ST90S, a high-throughput transmission fiber spectrometer meticulously designed for applications where signal-to-noise ratio and sensitivity are paramount. Optimized for 532 nm excitation systems, the ST90S delivers outstanding optical performance, making it the perfect instrument for gas Raman spectroscopy, advanced material analysis, and cutting-edge research.
The ST90S's core advantage stems from its use of a VPH volume holographic transmission grating, which achieves a remarkable diffraction efficiency of 90%. This key component is the foundation of a high-throughput optical path (Numerical Aperture 0.25) that maximizes light collection. Consequently, the system offers sensitivity that is five times greater than that of standard reflective spectrometers. This enhanced light gathering power is critical for detecting weak Raman scatterers, such as gases, enabling the capture of clear, detailed spectra even with brief acquisition times, as demonstrated by its capability to acquire a 1-second air Raman spectrum with a 5W laser.
Complementing the optical front end is a research-grade Andor iVac 316 deep-cooling area array CCD. This detector is specifically chosen for its high quantum efficiency and exceptionally low dark current, ensuring an outstanding signal-to-noise ratio. This allows the ST90S to resolve fine spectral details with a resolution down to 4 cm⁻¹, covering a broad spectral range from 260 to 4200 cm⁻¹. The instrument provides clean, high-fidelity data essential for accurate qualitative and quantitative analysis in demanding fields like online gas detection, chemical process monitoring, and biomedical research.
Built for reliability, the ST90S features a zero-aberration design that guarantees diffraction-limited imaging performance. Its robust construction ensures high stability for both laboratory and industrial environments. With flexible input options including SMA905 and Φ10mm multi-core fiber interfaces, it readily adapts to various integration needs. For scientists and engineers who require a spectrometer that combines high throughput, exceptional signal purity, and robust performance, the ST90S stands as a superior and reliable solution.
Technical Parameters:
| |
Performance Indicators |
Parameters |
| Detector |
- |
See model table for details |
Optical
Parameters |
Wavelength Range |
ST90S1: 540nm~686nm corresponds to 260~4200cm-1
ST90S2: 532nm~670nm corresponds to 0~3850cm-1 |
| Optical Resolution(ST90S1) |
0.25nm, corresponds to 8cm-1(50μm slit)
0.14nm, corresponds to 5cm-1(25μm slit) |
| Grating Type |
VPH volume holographic transmission grating |
| Diffraction Efficiency |
>85% |
| Fiber Interface |
SMA905 or Φ10mm multi-core optical fiber |
| Numerical Aperture |
0.25 |
Electrical
Parameters |
Integration Time |
1ms-3600s |
| Data Output Interface |
USB2.0 |
| ADC Bit Depth |
16-bit |
| Power Supply |
DC12V (ST90S1~ST90S4)
DC5V (ST90S5) |
| Operating Current |
3A (typical value 2A) |
| Operating Temperature |
-20°C ~60°C |
| Storage Temperature |
-30°C ~70°C |
| Operating Humidity |
<90%RH (no condensation) |
Physical
Parameters |
Dimensions |
348.7mm × 222.8mm × 126mm |
| Weight |
<6kg (including camera) |
Product Model List:
| Product Model |
ST90S1 |
ST90S2 |
ST90S3 |
ST90S4 |
Detector Brand
or Model |
AndoriVac 316 |
PI PIXIS 100BX |
Raptor261FI |
Raptor261BI |
| Chip Type |
Deep depletion of
back illuminated |
Back
illuminated |
Front
illuminated |
Back
illuminated |
Quantum
Efficiency |
80%@600nm |
90%@600nm |
45%@600nm |
80%@600nm |
| Number of Pixels |
2000*256 |
1340*100 |
2048*256 |
2048*256 |
| Pixel Size (μm) |
15*15 |
20*20 |
15*15 |
15*15 |
| Image Area (mm) |
30*3.8 |
26.8*2.0 |
30*3.8 |
30*3.8 |
Cooling
Temperature (℃) |
-70 |
-80 |
-70 |
-70 |
| * Customization available for other ranges |
Applications:
The JINSP ST90S spectrometer is perfect for a variety of application occasions and scenarios. It has a wavelength range of 540nm~686nm, which corresponds to 260~4200cm-1. The product category is fiber optic spectrometers, and it weighs less than 6kg (including camera). The numerical aperture is 0.25, and the integration time ranges from 1ms-3600s.
One of the most common scenarios where the JINSP ST90S is used is in 532 Confocal Raman microscopy. This technique is used to study the chemical and structural properties of molecules. The ultra-high resolution spectrometer makes it possible to detect even the smallest signals with great precision, which is essential for this type of research.
Overall, the JINSP ST90S is a versatile and reliable spectrometer that can be used in a variety of applications. Its ultimate sensitivity and high resolution make it a valuable tool for researchers and scientists who need to study the properties of molecules in great detail.
Support and Services:
The High-Throughput Transmission Fiber Spectrometer is a state-of-the-art product that provides reliable and accurate spectral analysis for a wide range of applications. Our product technical support and services include:
- Regular software updates and upgrades to ensure compatibility with the latest technologies
- Calibration and maintenance services to optimize performance and accuracy
- Customization options to meet specific application requirements
Our team of experienced professionals is dedicated to providing exceptional customer service and ensuring that our customers receive the highest level of support and satisfaction.
Packing and Shipping:
The High-Throughput Transmission Fiber Spectrometer comes in a sturdy cardboard box to ensure safe delivery.
FAQ:
1.What is the brand name of the product?
JINSP is our brand name.
2.What is the model number of the product?
ST90S Transmission Imaging Spectrometer.
3.What is the minimum order quantity for the product?
The minimum order quantity is 1 PC.
4.What are the payment terms for the product?
The payment terms are T/T and Western Union.
5.What is the delivery time for the product?
The delivery time is 40-70 working days.
